921 research outputs found

    Deep inelastic scattering and "elastic" diffraction

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    We examine the total cross section of virtual photons on protons, σγp(W2,Q2)\sigma_{\gamma^* p}(W^2,Q^2), at low xQ2/W21x \cong Q^2/W^2 \ll 1 and its connection with ``elastic'' diffractive production γT,LpXT,LJ=1p\gamma^*_{T,L}p \to X^{J=1}_{T,L} p in the two-gluon exchange dynamics for the virtual forward Compton scattering amplitude. Solely based on the generic structure of two-gluon exchange, we establish that the cross section is described by the (imaginary part of the) amplitude for forward scattering of qqˉq \bar q vector states, (qqˉ)T,LJ=1p(qqˉ)T,LJ=1p(q \bar q)^{J=1}_{T,L} p \to (q \bar q)^ {J=1}_{T,L} p. The generalized vector dominance/color dipole picture (GVD/CDP) is accordingly established to only rest on the two-gluon-exchange generic structure. This is explicitly seen by the sum rules that allow one to directly relate the total cross section to the cross section for elastic diffractive forward production, γT,Lp(qqˉ)T,LJ=1p\gamma^*_{T,L} p\to (q \bar q)^{J=1}_{T,L} p, of vector states.Comment: 24 pages, latex file with three eps figures. BI-TP 2002/2

    Regge residues from DGLAP evolution

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    We show that combining forward and backward evolution allows to extract the residues of the triple-pole pomeron and of the other singularities for 10 GeV2Q21000^2 \le Q^2 \le 1000 GeV2^2. In this approach, the essential singularity generated by the DGLAP evolution is considered as a numerical approximation to a triple-pole pomeron. Using an analytical expression for the form factors, we reproduce the experimental data with a χ2/dof\chi^2/dof of 1.02. This proves the compatibility between Regge theory and DGLAP evolution. The method used here enables us to evaluate the uncertainties on the gluon distribution which prove to be large at small xx and small Q2Q^2.Comment: 11 pages, 9 figures, RevTeX 4, Submitted to Phys. Re

    W Boson Inclusive Decays to Quarkonium at the LHC

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    In this paper, the production rates of quarkonia eta_c, J/psi, eta_b, Upsilon, B_c and B_c^* through W boson decay at the LHC are calculated, at the leading order in both the QCD coupling constant and in v, the typical velocity of the heavy quark inside of mesons. It shows that a sizable number of quarkonia from W boson decay will be produced at the LHC. Comparison with the predictions by using quark fragmentation mechanism is also discussed. Results show that, for the charmonium production through W decay, the difference between predictions by the fragmentation mechanism and complete leading order calculation is around 3%, and it is insensitive to the uncertainties of theoretical parameters; however, for the bottomonium and B_c^(*) productions, the difference cannot be ignored as the fragmentation mechanism is less applicable here due to the relatively large ratio mb/mw.Comment: Updated to match the published version in EPJ

    PDF and scale uncertainties of various DY distributions in ADD and RS models at hadron colliders

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    In the extra dimension models of ADD and RS we study the dependence of the various parton distribution functions on observable of Drell-Yan process to NLO in QCD at LHC and Tevatron energies. Uncertainties at LHC due to factorisation scales in going from leading to next-to-leading order in QCD for the various distributions get reduced by about 2.75 times for a μF\mu_F range 0.5 Q<μF<1.5 Q0.5 ~Q < \mu_F < 1.5 ~Q. Further uncertainties arising from the error on experimental data are estimated using the MRST parton distribution functions.Comment: 27 pages, 11 figures, the version to appear in European Physical Journal

    The Gluon Impact Factors

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    We calculate in the next-to-leading approximation the non-forward gluon impact factors for arbitrary color state in the tt-channel. In the case of the octet state we check the so-called "second bootstrap condition" for the gluon Reggeization in QCD, using the integral representation for the impact factors. The condition is fulfilled in the general case of an arbitrary space-time dimension and massive quark flavors for both helicity conserving and non-conserving parts.Comment: 32 pages, LaTeX, 1 EPS figure, uses epsf.sty and axodraw.st

    DGLAP evolution extends the triple pole pomeron fit

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    We show that the triple pole pomeron model \cite{CMS} provides an initial condition for a DGLAP evolution \cite{DGLAP} that produces a fit to high Q2Q^2 experimental DIS data. We obtain good χ2\chi^2 for initial scales down to 3 GeV2^2. Values of the initial scale smaller than 1.45 GeV2^2 are ruled out at the 90% confidence level.Comment: 8 pages, 6 figures, uses RevTex 4. Typos corrected, some points clarifed and 1 figure adde

    Bounds on the dipole moments of the tau-neutrino via the process e+eννˉγe^{+}e^{-}\rightarrow \nu \bar \nu \gamma in a 331 model

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    We obtain limits on the anomalous magnetic and electric dipole moments of the ντ\nu_{\tau} through the reaction e+eννˉγe^{+}e^{-}\rightarrow \nu \bar \nu \gamma and in the framework of a 331 model. We consider initial-state radiation, and neglect WW and photon exchange diagrams. The results are based on the data reported by the L3 Collaboration at LEP, and compare favorably with the limits obtained in other models, complementing previous studies on the dipole moments.Comment: 13 pages, 4 figures, to be published in The European Physical J C. arXiv admin note: substantial text overlap with arXiv:hep-ph/060527

    Supersymmetry without R-parity : Constraints from Leptonic Phenomenology

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    R-parity conservation is an {\it ad hoc} assumption in the most popular version of the supersymmetric standard model. Most studies of models which do allow for R-parity violation have been restricted to various limiting scenarios. The single-VEV parametrization used in this paper provides a workable framework to analyze phenomenology of the most general theory of SUSY without R-parity. We perform a comprehensive study of leptonic phenomenology at tree-level. Experimental constraints on various processes are studied individually and then combined to yield regions of admissible parameter space. In particular, we show that large R-parity violating bilinear couplings are not ruled out, especially for large tanβ\tan\beta.Comment: 56 pages Revtex with figures incorporated; typos (including transcription typo in Table II) and minor corrections; proof-read version, to appear in Phys. Rev.

    Observation of Scaling Violations in Scaled Momentum Distributions at HERA

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    Charged particle production has been measured in deep inelastic scattering (DIS) events over a large range of xx and Q2Q^2 using the ZEUS detector. The evolution of the scaled momentum, xpx_p, with Q2,Q^2, in the range 10 to 1280 GeV2GeV^2, has been investigated in the current fragmentation region of the Breit frame. The results show clear evidence, in a single experiment, for scaling violations in scaled momenta as a function of Q2Q^2.Comment: 21 pages including 4 figures, to be published in Physics Letters B. Two references adde

    Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in √s = 7 TeV pp collisions with the ATLAS detector

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    A search for the direct production of charginos and neutralinos in final states with three electrons or muons and missing transverse momentum is presented. The analysis is based on 4.7 fb−1 of proton–proton collision data delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in three signal regions that are either depleted or enriched in Z-boson decays. Upper limits at 95% confidence level are set in R-parity conserving phenomenological minimal supersymmetric models and in simplified models, significantly extending previous results
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